Chapter 13: Problem 61
Reverse the order of integration in the following integrals. $$\int_{0}^{1} \int_{0}^{\cos ^{-1} y} f(x, y) d x d y$$
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Chapter 13: Problem 61
Reverse the order of integration in the following integrals. $$\int_{0}^{1} \int_{0}^{\cos ^{-1} y} f(x, y) d x d y$$
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A disk of radius \(r\) is removed from a larger disk of radius \(R\) to form an earring (see figure). Assume the earring is a thin plate of uniform density. a. Find the center of mass of the earring in terms of \(r\) and \(R\) (Hint: Place the origin of a coordinate system either at the center of the large disk or at \(Q\); either way, the earring is symmetric about the \(x\) -axis.) b. Show that the ratio \(R / r\) such that the center of mass lies at the point \(P\) (on the edge of the inner disk) is the golden mean \((1+\sqrt{5}) / 2 \approx 1.618\)
Spherical to rectangular Convert the equation \(\rho^{2}=\sec 2 \varphi\) where \(0 \leq \varphi<\pi / 4,\) to rectangular coordinates and identify the surface.
Mass from density Find the mass of the following solids with the given density functions. Note that density is described by the function \(f\) to avoid confusion with the radial spherical coordinate \(\rho\). The ball of radius 8 centered at the origin with a density \(f(\rho, \varphi, \theta)=2 e^{-\rho^{3}}\)
Miscellaneous volumes Choose the best coordinate system for finding the volume of the following solids. Surfaces are specified using the coordinates that give the simplest description, but the simplest integration may be with respect to different variables. The wedge cut from the cardioid cylinder \(r=1+\cos \theta\) by the planes \(z=2-x\) and \(z=x-2\)
Gravitational field due to spherical shell A point mass \(m\) is a distance \(d\)
from the center of a thin spherical shell of mass \(M\) and radius \(R .\) The
magnitude of the gravitational force on the point mass is given by the
integral
$$F(d)=\frac{G M m}{4 \pi} \int_{0}^{2 \pi} \int_{0}^{\pi} \frac{(d-R \cos
\varphi) \sin \varphi}{\left(R^{2}+d^{2}-2 R d \cos \varphi\right)^{3 / 2}} d
\varphi d \theta$$
where \(G\) is the gravitational constant.
a. Use the change of variable \(x=\cos \varphi\) to evaluate the integral and
show that if \(d>R,\) then \(F(d)=\frac{G M m}{d^{2}},\) which means the force is
the same as if the mass of the shell were concentrated
at its center.
b. Show that if \(d
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